Concept:
• In a standard Young's Double Slit Experiment (YDSE), the sources are exactly in phase (initial phase difference = $0$). At the center of the screen, the path lengths from both slits are equal ($\Delta x = 0$).
• This zero path difference normally results in a net phase difference of zero, leading to constructive interference (a central bright maximum).
• The total phase difference $\Delta \phi$ at any point on the screen is the sum of the initial phase difference $\phi_0$ and the phase difference due to the path difference ($\frac{2\pi}{\lambda} \Delta x$).
Step 1: Analyze the new phase condition at the center
The problem states that the waves emitted from slits $S_1$ and $S_2$ now have an inherent initial phase difference, $\phi_0 = \pi$ radians.
At the exact geometric center of the screen, the distance travelled by the light from both slits is perfectly identical.
Therefore, the path difference at the center is still zero: $\Delta x = 0$.
The phase difference created by the path length difference is:
\[ \phi_{path} = \frac{2\pi}{\lambda} \times \Delta x = \frac{2\pi}{\lambda} \times 0 = 0 \text{ radians} \]
Step 2: Calculate the total effective phase difference
The total phase difference $\Delta \phi$ at the central point is:
\[ \Delta \phi = \phi_0 + \phi_{path} \]
\[ \Delta \phi = \pi + 0 = \pi \text{ radians} \]
Step 3: Determine the nature of interference
When the total phase difference between two superimposing waves is an odd multiple of $\pi$ (e.g., $\pi, 3\pi, 5\pi$), they are completely out of phase.
This condition strictly leads to destructive interference.
Because destructive interference minimizes intensity, a dark spot will be formed.
Step 4: Conclusion
Instead of a central bright fringe, a central dark fringe (minimum) will be obtained on the screen. The entire interference pattern will effectively shift, swapping the positions of all maxima and minima.